RECONSTRUCTION OF EXTREMELY DENSE BREAST COMPOSITION
UTILIZING INVERSE SCATTERING TECHNIQUE INTEGRATED WITH
FREQUENCY-HOPPING APPROACH
Ng Shi Wei1, Kismet Anak Hong Ping1, Lim Sin Yee1, Wan Azlan Bin Wan Zainal Abidin1, Toshifumi Moriyama2 and Takashi Takenaka2
1Department of Electrical and Electronic Engineering, Faculty of Engineering, Universiti Malaysia, Kota Samarahan, Sarawak, Malaysia 2Department of Electrical and Electronic Engineering, Faculty of Engineering, Nagasaki University, Bunkyo-machi, Nagasaki , Japan
E-Mail: [email protected]
ABSTRACT
The Forward-Backward Time-Stepping (FBTS) inverse scattering technique is utilized for breast composition reconstruction of an extremely dense breast model at different center frequencies. A numerical extremely dense breast phantom is used and resized to suit the Finite-Difference Time-Domain (FDTD) lattice environment utilizing two-dimensional (2-D) FBTS technique. The average value of fibro glandular region for reconstruction with Frequency-hopping approach applied is much closer to average value of the actual image compared to the reconstruction without Frequency-approach applied. Hence, the composition of the extremely dense breast model can be reconstructed with Frequency-hopping approach is applied and the details of the reconstruction is also enhanced.
Keywords: breast imaging, frequency-hopping, inverse scattering.
INTRODUCTION
In developed country, breast cancer is a top ranked cancer although it is rare in men (DeSantis et al.
2014). Based on the findings, breast cancer ranks first among the women especially women aged between 20 to 59 years old. According to the breast cancer mortality trend, there will be 40,430 expected deaths caused by breast cancer which includes 40,000 women and 430 men as reported in Siegel et al. (2014). Therefore, annually breast screening is essential for early breast cancer detection and proper treatment to reduce the breast cancer mortality.
Clinical breast examination and mammography are the common breast screening methods for women at average risk. X-ray mammography is the standard screening method for breast tumour detection (Champaign and Cederbom, 2000). Based on the studies on mammography, radiologists recommended depicting the severity by using the American College of Radiology’s (ACR) Breast Imaging Reporting and Data System (BI-RADS). BI-RADS becomes the standard in the mammographic density assessment (Liberman, 2002).
According to the studies in Tabar and Dean (2010), it indicated that the breast density is one of the risk factors causing missed cancers (positive and false-negative) in mammographic interpretations especially on dense breasts. The sensitivity of the X-ray screening mammography is lower for women with heterogeneously dense or very dense breasts according to Joy et al. (2005). In Kolb et al. (2002) stated that more than 11,000 women without clinical symptoms of breast cancer, the sensitivity of mammography was only 48% for the extremely dense breasts compared to the entire sample of women with 78% sensitivity.
The mentioned limitations have demonstrated a weighty challenge to the accuracy of early detection of breast cancer. It is also contributing to the alternative detection techniques by many researchers (Li and Hagness, 2001), (Hassan and El-Shenawee, 2011). The nonionizing microwave breast imaging is rationale due to the significant contrast in the dielectric properties of normal breast tissue and malignant tumours (Chaudhary et al. 1984). There are various types of active microwave approaches utilizing frequency-domain inverse scattering (Qianqian et al. 2004) and ultra-wideband (UWB) radar-based techniques (Li et al. 2004) for breast imaging. These approaches demonstrated that the tumours can be detected both in phantom experiments and numerical studies (Ping
et al. 2009). Furthermore, time-domain scattering data
contains more information as compared to frequency-domain scattering data. Hence, electromagnetic imaging in time-domain has the potential to reconstruct electrical profiles more accurately.
METHODOLOGY
Forward-backward time-stepping technique
The Forward-Backward Time-Stepping (FBTS) technique utilizes the broadband microwave signals to solve the inverse scattering problems in time domain. It possesses the potential to reconstruct images which provide useful quantitative information about the location, shape and the internal composition of the breast.
The aim of this technique is to determine the shape, location and electric properties of any electromagnetic inverse scattering problem. The electric properties include the permittivity, permeability, electric conductivity and magnetic conductivity. Figure-1 shows a typical configuration of an active microwave tomography setup for FBTS inverse scattering problem. The breast is assumed to be embedded in a free space. The breast is illuminated successively by M short pulsed waves generated by current sources located at
.
Figure-1. Configuration of the FBTS in 2-D FDTD scheme.
The major challenge in solving inverse scattering problem is reconstructing the electric properties’ profile utilizing the knowledge of the transient field data measured at several observation points
for each illumination. For the initial condition, the currents are assumed to be generated at time t=0 and there are no electromagnetic fields found before time t=0. Hence, the total electromagnetic fields for the mth current source
satisfy the following Maxwell’s equation:
(1)
Under zero initial condition for
(2)
To initialize the FBTS procedure, an optimization problem is formulated in the form of cost functional to be minimized.
(3) where p is a medium parameter vector function as expressed in Equation (3), is a non-negative weighting function which takes a value of zero at time t=T
(T is the time duration of the measurement), and and are the calculated electromagnetic fields for an estimated medium parameter vector p and the measured electromagnetic fields due to
mth source, respectively.
Frequency-hopping approach
Frequency-hopping approach is utilized to process multi-frequency microwave measurement data. This approach can be used to reconstruct larger dielectric bodies for microwave imaging with higher fidelity compared to a single-frequency reconstruction. This approach uses only data at a few selected frequencies leads to reduce data acquisition time in a practical system. The frequency of the illuminating field is increased for a better resolution of the reconstructed image. For large structures or high-contrast objects, they can be imaged at lower frequencies while higher frequency of the illuminating field are used for the reconstruction of high-contrast normal breast tissues by interpreting the initial guess from the resultant result of the reconstruction at lower frequency for the proceeding iterations. Hence, frequency-hopping approach can be used for the reconstruction of large structures or high-contrast normal breast tissues.
Numerical breast phantom
SIMULATION SETUP
Reconstruction of a 2-D numerical extremely dense breast model is done to demonstrate the validity of the FBTS technique to reconstruct the composition of extremely dense breast model. There are 16 antennas utilized in this work as shown in Figure-1. Each antenna will become transmitter sequentially to transmit a pulse while the remaining 15 antennas will become receivers to collect the scattered fields in the FDTD lattice environment. A sinusoidal modulated Gaussian pulse with different center frequencies is excited by the transmitter into the FDTD lattice environment. The FDTD lattice environment is surrounded by Convolutional Perfectly Matched Layer (CPML) to prevent the reflection of the signal at the boundary of the environment.
The entire FDTD lattice environment is set as free space with relative permittivity, and conductivity, . The breast model is then simulated at different center frequencies from 1GHz until 4GHz. The frequency-hopping approach is applied in order to enhance the resolution of the reconstruction of the breast model’s dielectric properties.
Figure-2. Actual relative permittivity of the numerical breast model.
RESULTS AND DISCUSSION
Figure-3 and Figure-4 show the reconstructed images of an extremely dense breast utilizing FBTS
technique. The relative permittivity of this breast can be reconstructed roughly at center frequency of 1GHz as illustrated in Figure 3(a) and Figure 4(a), respectively. The average value of the relative permittivity for the fibro glandular region are = 37.287 (coronal slice 100)
and = 37.663 (coronal slice 120), which are
significantly lower than the actual values of = 40.061
(coronal slice 100) and =40.394 (coronal slice 120).
In comparing Figure-3(a) to Figure-3(d), the fibro glandular region of the extremely dense breast model only can be estimated at center frequency of 1GHz. However, the finer details or smaller region of the fibro glandular region cannot be reconstructed. This shows that lower frequency only able to reconstruct the larger region of the extremely dense breast composition. Therefore, higher frequency is required in order to reconstruct the small region. However, the composition of the extremely dense breast was unsuccessfully reconstructed due to the effect of nonlinearity in the optimization procedure. Hence, the Frequency-hopping approach is applied to improve resolution of the reconstruction and overcome the effect of nonlinearity.
From the results obtained as in Figure-5(a) and Figure-6(a), Frequency-hopping approach is applied from 1GHz to 2GHz with the average values of the relative permittivity for the fibro glandular region are =
37.6143 (coronal slice 100) and = 38.1619 (coronal
slice 120), which are closer to the actual values of =
39.513 (coronal slice 100) and =39.84 (coronal slice
120) compared to the reconstruction using single center frequency with average value of fibro glandular region of = 34.615 (coronal slice 100) and =31.487
(coronal slice 120), respectively.
As shown in Table-1 and Table-2, the average values for the fibro glandular region are getting closer to the actual images as the center frequency increases by applying the Frequency-hopping approach.
The composition of the extremely dense breast can be reconstructed significantly compared to the reconstruction using a single center frequency only. This shows that the effect of nonlinearity of the local optimization approach can be overcome by utilizing Frequency-hopping approach. This is also proven that Frequency-hopping approach enables the FBTS to estimate the large region of fibro glandular at lower frequency and estimate the smaller region of fibro glandular at higher frequency.
between the dielectric properties of the tumour and fibro glandular region is small.
The results obtained in Figure-3 and Figure-4 show the images cannot be reconstructed with the center frequency above than 2GHz due to the huge difference of
the dielectric properties of the fibro glandular tissues and fatty tissues. Hence, Frequency-hopping approach is needed to reconstruct the low contrast numerical breast model.
Figure-3. Reconstruction of relative permittivity using FBTS technique at different frequencies (Coronal Slice 100).
Table-1. The average value of reconstructed breast model (Coronal Slice 100).
Table-2. The average value of reconstructed breast model (Coronal Slice 120).
Figure-5. Reconstruction of relative permittivity using FBTS technique with Frequency-hopping approach applied at different frequencies (Coronal Slice 100).
Figure-6. Reconstruction of relative permittivity using FBTS technique with Frequency-hopping approach applied at different frequencies (Coronal Slice 120).
CONCLUSION
The iterative FBTS algorithm can be used to solve the inverse scattering problem using broadband microwave signal in time domain for breast composition reconstruction. The composition of an extremely dense
breast model can be reconstructed with the integration of Frequency-hopping approach into iteration FBTS algorithm.
by implanting different size of tumour into the fibro glandular region of the numerical breast model.
ACKNOWLEDGEMENTS
This research was supported by OSAKA GAS Foundation in Cultural Exchange (OGFICE) Research Grant Scheme.
REFERENCES
[1] Champaign J. L. and Cederbom G. J. 2000. Advances in Breast Cancer Detection with Screening Mammography. Ochsner J., Vol. 2, No. 1, pp. 33-35.
[2] Chaudhary S. S., Mishra R. K., Swarup A. and Thomas J. M. 1984. Dielectric properties of normal & malignant human breast tissues at radiowave & microwave frequencies. Indian J. Biochem. Biophys., Vol. 21(1), pp. 76-79.
[3] Carol DeSantis, Jiemin Ma, Leah Bryan and Ahmedin Jemal. 2014. Breast cancer statistics. CA: A Cancer Journal for Clinicians, Vol. 64, No. 1, pp. 52-62.
[4] Ahmed M. Hassan and Magda El-Shenawee. 2011. Review of Electromagnetic Techniques for Breast Cancer Detection. IEEE Reviews in Biomedical Engineering, Vol. 4, pp. 103-118.
[5] Johnson J.E., Takenaka T. and Tanaka T. 2008. Two-dimensional Time-domain Inverse Scattering for Quantitative Analysis of Breast Composition. IEEE Trans. Biomed. Eng. Vol. 55, No. 8, pp. 1941-1945.
[6] Janet E. Joy, Edward E. Penhoet Diana, B. Petitti. Editors and Institute of Medicine and National Research Council Committee on New Approaches to Early Detection and Diagnosis of Breast Cancer. (2005). Benefits and Limitations of Mammography. Saving Women's Lives: Strategies for Improving Breast Cancer Detection and Diagnosis. Washington (DC), National Academies Press (US), pp. 37-62.
[7] Kolb T. M., Lichy J. and Newhouse J. H. 2002. Comparison of the performance of screening mammography, physical examination, and breast US and evaluation of factors that influence them: an analysis of 27,825 patient evaluations. Radiology, Vol. 225, No. 1, pp. 165-175.
[8] University of Wisconsin Cross-Disciplinary Electromagnetics Laboratory. UWCEM numerical breast phantoms repository [Online]. Available: http://uwcem.ece.wisc.edu/MRIdatabase/index.html
[9] Xu Li, Shakti K. Davis, Susan C. Hagness, Daniel W. van der Weide and Barry D. Van Veen. 2004. Microwave imaging via space-time beamforming: Experimental investigation of tumor detection in multilayer breast phantoms. Microwave Theory and Techniques, Vol. 52, No. 8, pp. 1856-1865.
[10] Xu Li and Susan C. Hagness. 2001. A Confocal Microwave Imaging Algorithm for Breast Cancer Detection. IEEE Microwave and Wireless Components Letters, Vol. 11, No. 3, pp. 130-132.
[11] Liberman L. 2002. Breast imaging reporting and data system (BI-RADS). Radiologic Clinics of North America, Vol. 40, No. 3, pp. 409-430.
[12] Ping K. A. H., Moriyama T., Takenaka T. and Tanaka T. 2008. Reconstruction of breast composition in a free space utiizing 2-D forward-backward time-stepping for breast cancer detection. Advances in Medical, Signal and Information Processing (MEDSIP), 4th lET Intematioal Conf., pp. 1-4.
[13] Kismet Anak Hong Ping, Toshifumi Moriyama, Takashi Takenaka and Toshiyuki Tanaka (2009). Two-dimensional Forward-Backward Time-Stepping approach for tumor detection in dispersive breast tissues. Microwave Symposium (MMS), 2009 Mediterrannean, pp. 1-4.
[14] Qianqian F., Meaney P., Geimer S., Streltsov A. and Paaulsen K. 2004. Microwave image reconstruction from 3-D fields coupled to 2-D parameter estimation. IEEE Trans. Med. Imag., Vol. 23, No. 4, pp. 475-484.
[15] Rebecca Siegel, Jiemin Ma, Zhaohui Zou and Ahmedin Jemal 2014. Cancer statistics, 2014. CA: A Cancer Journal for Clinicians, Vol. 64, No. 1, pp. 9-29.
[16] Tabar L. and Dean P. B. 2010. A new era in the diagnosis and treatment of breast cancer. Breast J, 16 Suppl 1, pp. S2-4.